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Fig. 5.
Two particles of strengths
ω 1 and
ω 2 , carrying mollification kernels
ζ .
as illustrated in Fig. 5. The core size defines the characteristic
width of the kernel and thus the spatial resolution of the method.
The regularized function approximation is defined as
Ú
(3)
u
()
x
=
u
() (
y
z
x
-
y
)
d
y
and can be used to recover the function values at arbitrary loca-
tions x . The approximation error is of order r , hence
r
(4)
u
()
x
=
u
()
x
+
O
( ).
As introduced above, r is the first nonvanishing moment of the
mollification kernel. 27,85
For positive symmetric kernels, such as a
Gaussian, r
=
2.
Step 3: mollified integral discretization . The regularized integral in
Eq. (3) is discretized over N particles using the quadrature rule
N
(
)
 ω z
1
u h
h
h
()
x
=
x
-
x
,
(5)
p
p
p
=
where x p and ω p are the numerical solutions of the particle positions
and strengths, determined by discretizing the ODEs in Eq. (1) in
time. The quadrature weights ω p are the particle strengths and
depend on the particular quadrature rule used. The most frequent
choice is to use midpoint quadrature, 102
thus setting ω p
=
u ( x p ) V p ,
 
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